Catalytic Activity of AuCu Clusters on MgO(100) - ACS Publications

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Catalytic Activity of AuCu Clusters on MgO(100): Effect of Alloy Composition for CO Oxidation Li Ma,†,‡ Kari Laasonen,§ and Jaakko Akola*,†,‡,∥ †

Department of Physics, Tampere University of Technology, FI-33101 Tampere, Finland COMP Centre of Excellence, Department of Applied Physics, Aalto University, FI-00076 Aalto, Finland § COMP Centre of Excellence, Department of Chemistry, Aalto University, FI-00076 Aalto, Finland ∥ Department of Physics, Norwegian University of Science and Technology, NO-7491 Trondheim, Norway ‡

S Supporting Information *

ABSTRACT: Density functional simulations have been performed for Au7Cu23 and Au23Cu7 clusters on MgO(100) supports to probe their catalytic activity for CO oxidation. The adsorption of reactants, O2 and CO, and potential O2 dissociation have been investigated in detail by tuning the location of vacancies (F-center, V-center) in MgO(100). The total charge on Au7Cu23 and Au23Cu7 is negative on all supports, regardless of the presence of vacancies, but the effect is significantly amplified on the Fcenter. Au7Cu23/MgO(100) and Au23Cu7/MgO(100) with an F-center are the only systems to bind O2 more strongly than CO. In each case, O2 can be effectively activated upon adsorption and dissociated to 2 × O atoms. The different reaction paths based on the Langmuir−Hinshelwood (LH) and Eley−Rideal (ER) mechanisms for CO oxidation have been explored on the Au7Cu23 and Au23Cu7 clusters on F-centers, and the results are compared with the previous findings for Au15Cu15. Overall, the reaction barriers are small, but the changes in the Au:Cu ratio tune the reactant adsorption energies and sites considerably, showing also varying selectivity for CO and O2. The microkinetic model built on the basis of the above results shows a pronounced CO2 production rate at low temperature for the clusters on F-centers.

1. INTRODUCTION Bimetallic clusters have caught considerable attention over the past decade, since they provide the possibility to tailor the size and the composition of nanocatalyst systems. The synergetic effects between different metals can eventually result in a material with enhanced catalytic properties.1−6 Generally, the synergy arises from interactions among metals, which can modify the electronic or structural properties of the active sites. Gold nanoparticles supported on metal oxides have been proven to be highly active and selective catalysts for a variety of chemical reactions.7 One of the most notable example is the reaction of CO oxidation at low temperature.8−10 However, most Au catalysts still suffer from rapid deactivation, which is a drawback for practical applications. The deactivation mechanism is often attributed to the sintering of Au particles.11,12 Correspondingly, it is challenging to prepare small gold nanoparticles on inert supports (e.g., SiO2, Al2O3, MgO) without anchoring sites (e.g., defects, F-centers). It has also © XXXX American Chemical Society

been reported that the F-center on the MgO surface plays a critical role in the activation of Au catalysts.13,14 High catalytic activity for clusters with more than eight gold atoms has been demonstrated by experiments for the CO oxidation on selected Aun clusters deposited on defect-rich MgO(100) films at low temperatures.13 The adsorption and activation of O2 are important steps in the CO oxidation reaction,15 and the oxide support is supposed to affect the activation of oxygen.16,17 The catalytic activity of Au nanoparticles is significantly reduced on inert substrates, which cannot facilitate strong adsorption for O2 molecules and results in high O2 dissociation barriers. Here, Special Issue: ISSPIC XVIII: International Symposium on Small Particles and Inorganic Clusters 2016 Received: November 30, 2016 Revised: February 15, 2017 Published: February 17, 2017 A

DOI: 10.1021/acs.jpcc.6b12054 J. Phys. Chem. C XXXX, XXX, XXX−XXX

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The Journal of Physical Chemistry C

the surface and how this couples to the properties of the metal−oxide interface and the MgO(100) surface itself.

alloying with a second metal is an effective way to improve the capability of Au to activate molecular oxygen, and, for example, Cu can play such a role.18 Catalysts based on Au−Cu alloys have been reported as promising and effective catalysts for low temperature CO oxidation because of the synergistic interaction between Cu and Au.19,20 They exhibit higher activity and resistance against sintering in comparison to monometallic Au catalysts. In practice, a number of factors influence the catalytic performance of bimetallic nanoparticles, e.g., nanostructure, composition, size, and the chemical structure of the support (including defects). Thus, the catalytic process is a complex problem. Concerning nanoparticle composition, there is controversy of the effect of the Au/Cu ratio for the activity toward CO oxidation. Mozer et al.21 found a correlation between activity and Cu loading of an alumina-supported Au catalyst. While low amounts of copper were beneficial for the CO oxidation activity, high copper contents caused blocking of the Au active sites, thus decreasing the catalytic activity. However, Sandoval et al.20 reported the highest activity of CO oxidation for AuCu/TiO2 catalyst with a somewhat higher Au:Cu ratio of 1:0.9. Moreover, the effect of redox treatments on AuCu nanoparticles is also a matter of controversy in experimental studies.22−24 AuCu systems have three ordered alloys in the bulk: Au0.5Cu0.5 (fcc, L10), Au0.25Cu0.75 (fcc, L12), and Au0.75Cu0.25 (fcc, L12), and experiments have shown that the stoichiometry of bulk alloys can be reproduced well also in AuCu clusters.25 Pauwels et al.26 reported AuCu clusters generated by laser vaporization and deposited at low kinetic energy on MgO substrate. The clusters were observed to adopt the truncated octahedral morphology. In particular, the clusters with the stoichiometric compositions Au0.25Cu0.75, Au0.5Cu0.5, and Au0.75Cu0.25 were all found to have an fcc structure and to be in a cube-on-cube epitaxy relation with MgO(100). To explore the catalytic activity of AuCu clusters, we have previously performed a systematic study of Au15Cu15 (1:1 composition) on MgO(100) with and without vacancies for CO oxidation.27 Our calculations revealed that O2 can be effectively activated upon adsorption and dissociated to 2 × O atoms easily. The reaction barriers were systematically lower for the substrate with an F-center. Here, we aim to investigate how the cluster composition itself affects these results, and we concentrate on two AuCu clusters (1:3 and 3:1) with the same size and pyramidal shape (fcc). As shown by Ferrando et al. by using the global optimization search and density functional theory (DFT) calculations,28 the fcc pyramidal structure is energetically favorable for 30-atom AuCu clusters on MgO(100). We use DFT combined with a microkinetic model to elucidate the CO oxidation reaction mechanism on the MgO-supported Au7Cu23 and Au23Cu7 clusters and demonstrate the effect of the Au/Cu ratio and the role of vacancies in the MgO(100) support. Although the associated formation energies are high, experimental studies have shown that the vacancies or defect sites exist on the MgO(100) single crystal surface,29−33 which is either cleaved or grown on a metal support in ultrahigh vacuum. Furthermore, such defect sites can be generated by Ar sputtering, and they have been generally considered as the main anchoring sites in the nucleation and growth of metal particles or thin films.29,34,35 Previously, many experimental and theoretical studies have been devoted to single metal/MgO(100) systems.29,36−42 The key issues to understand have been how metal adatoms adsorb and grow on

2. COMPUTATIONAL METHOD The DFT calculations were performed using the CP2K program package.43,44 The exchange-correlation interaction was treated within the spin-polarized generalized gradient approximation with the functional form by Perdew−Burke− Ernzerhof (GGA-PBE).45 Gaussian and plane wave (GPW) basis sets were used to represent the Kohn−Sham orbitals and electron density. A molecularly optimized double-ζ valence plus polarization (DZVP) basis set46 was used for the Gaussian expansion of the wave functions. Herein, the basis set superposition error (BSSE) has been reduced during the basis set optimization. The complementary plane wave basis set has a 600 Ry energy cutoff for the calculation steps involving electron density. The description of the valence electron−ion interaction is based on the analytic pseudopotentials derived by Goedecker, Teter, and Hutter (GTH).47 The MgO(100) substrate was modeled by a four-layer slab with 36 Mg and 36 O atoms in each layer (in total 288 atoms) and a vacuum layer of 20 Å. It has been previously shown that the relaxation of substrate atoms has very small effects during the optimization.28,48 The lower two layers of the substrate were held frozen at the optimal DFT lattice constant of 4.24 Å (experimental value 4.22 Å).48 The previously published26,28 fcc pyramidal geometries of Au7Cu23 and Au23Cu7 clusters were chosen as the model structures on MgO(100). To illustrate the effect of support vacancies, three cases were considered: an ideal MgO support (defect-free), MgO support having an Ovacancy (F-center), and MgO support with an Mg-vacancy (Vcenter). The energetically most favorable adsorption configurations of Au7Cu23 and Au23Cu7 on MgO(100) on vacancies were located by examining the different point defect sites with respect to the AuCu cluster position on MgO(100). The adsorption energies of Au7Cu23 and Au23Cu7 clusters (E1ad) on MgO(100) supports were computed as 1 Ead = E(AuCu) + E(MgO) − E(AuCu/MgO)

(1)

For the molecular and atomic adsorption of reactants on Au7Cu23/MgO and Au23Cu7/MgO, the adsorption energy (E2ad) of a given arrangement was computed as 2 Ead = E(AuCu/MgO) + E(adsorbant)

− E(AuCu/MgO + adsorbant)

(2)

Here, E(X) in eqs 1 and 2 is the total energy of the corresponding system X and AuCu refers to Au7Cu23 or Au23Cu7. We used the Bader method for evaluating the spatial atomic charge decomposition.49 The reaction pathways were mapped using the climbing image nudged elastic band (CI-NEB) method.50 The obtained minima and transition state structures were further identified by vibrational analysis. Zero-point energy (ZPE) corrections were systematically included in the energy and reaction barrier calculations. In addition, the hybrid DFT functionals (PBE0 and B3LYP) have been previously tested in our CO oxidation benchmarks on Cu clusters,51 where we observed that the energetic ordering of different reaction paths (barriers) remained the same, although the reaction barriers were systematically lower for GGA-PBE. Furthermore, the different spin states were checked for the MgO(100) substrate with F- and V-center defects. The energy of the B


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2.49−2.77 Å, respectively. The corresponding bond lengths of Au23Cu7 are in the range of 2.66−3.19, 2.62−2.91, and 2.63− 2.97 Å, respectively. The shape of the bottom layer of the Au7Cu23 cluster is a square with 4 Au atoms on the corners and 12 Cu atoms on the center and periphery. Upon adsorption, the Cu atoms directly above support O atoms move down, forming Cu−O bonds in the range of 2.11−2.43 Å, which are considerably shorter than the Au−O bonds (2.79−2.93 Å). For the square bottom layer of the Au23Cu7 cluster, 2 Cu atoms locate on the center forming Cu−O bonds of 2.21 Å, compared with the 14 Au−O bonds in the range of 2.59−2.76 Å. Bader charge analysis shows that Au7Cu23 and Au23Cu7 carry a net charge of −1.96 and −2.15 e, respectively, which indicates that MgO(100) has transferred charge (electrons) to the cluster. A detailed analysis of the atomic charges in Au7Cu23 shows that Au atoms gain electron density up to 0.60 e, while Cu atoms lose electron density up to 0.20 e. Similarly, for the Au23Cu7 cluster, Au atoms gain electron density up to 0.42 e while Cu atoms lose electron density up to 0.38 e. For the F-center support, the geometries of Au7Cu23 and Au23Cu7 change primarily by the downward movement of the corner Au atom toward the F-center (Cs) (Figure 1). The adsorption energies of Au7Cu23 and Au23Cu7 increase to 6.35 and 7.06 eV, and the clusters are pronouncedly negatively charged by total charges of −3.41 and −3.66 e, respectively. The Au atom above the F-center in Au7Cu23 is strongly negatively charged by −1.53 e, which considerably differs from the defect-free case (−0.58 e). The other Au atoms are negatively charged down to −0.63 e, while all Cu atoms are positively charged up to +0.20 e. Similarly, the Au atom above the F-center in Au23Cu7 is negatively charged by −1.20 e compared to the −0.24 e in the defect-free case. The charge transfer from the F-center has both local and nonlocal components, as approximately one-half of the charge transferred locates in the pointing Au atom and the rest is mainly distributed across the other Au atoms. For the V-center, the defect locates below the center of the bottom layer of Au 7 Cu 23 and Au 23 Cu 7 (Figure 1, C 2ν symmetry). The binding energies of Au7Cu23/MgO and Au23Cu7/MgO are the highest (9.55 and 7.78 eV) of all supports. Here, the triplet state was used for the V-center alone to take into account the correct spin state. The strong adsorption causes the Au−O and Cu−O bond lengths to decrease for both cases, while the charge transfer from the support is the smallest (Table 1). Such interaction with the support is advantageous because pinned AuCu clusters are less susceptible to deactivation due to thermal sintering. As analyzed for Au15Cu15/MgO(100),27 there is no direct relationship between the interaction energy and the charge transfer for AuCu/MgO systems. The amount of charge

singlet state is 1.34 eV lower than that of the triplet state for the F-center, whereas the triplet state is energetically 0.35 eV lower for the V-center. However, the energy of the singlet state is always lower than that of the triplet state once the AuCu clusters have been adsorbed on the substrate.

3. RESULTS AND DISCUSSION 3.1. Au7Cu23 and Au23Cu7 on MgO Supports. Figure 1 gives the most stable adsorption geometries of Au7Cu23 and

Figure 1. (top row) Optimized geometries of Au7Cu23/MgO(100) and Au23Cu7/MgO(100) and the corresponding MgO(100) surface (a dashed square denoting the cluster position) with the defect-free, Fcenter, and V-center support. (bottom row) Top view and angular view with one layer of support of the defect-free Au7Cu23/MgO(100) and Au23Cu7/MgO(100) geometries. Color key: yellow, Au; coral, Cu; green, Mg; red, O.

Au23Cu7 on three MgO(100) supports and the corresponding MgO(100) surfaces with assigned point defect sites. The adsorption energy, geometric parameters, and charge transfer between clusters and MgO(100) are listed in Table 1. The corresponding values for Au15Cu15/MgO27 are also included in Table 1 for comparison. On the defect-free MgO surface (Figure 1), the Au7Cu23 and Au23Cu7 clusters retain the symmetric (C2ν) fcc pyramidal structure with Au−O and Cu−O bonds between the AuCu/ MgO interface. The Au−Au, Cu−Cu, and Au−Cu bond lengths of Au7Cu23 are in the range of 2.82, 2.44−2.68, and

Table 1. Adsorption Energy (E1ad), Net Charge (Q), Bond Length of Cu−O (rCu−O) and Au−O (rAu−O), Average Metallic Bond Length ⟨R⟩, and Symmetry of the Au7C23, Au15Cu15, and Au23Cu7 Clusters on Three MgO(100) Supports

E1ad (eV) Q (e) rCu−O (Å) rAu−O (Å) ⟨R⟩ (Å) symmetry

defect-free

F-center

V-center

Au7Cu23/Au15Cu15/Au23Cu7



4.95/5.42/4.71 −1.96/−1.96/−2.15 2.11−2.43/2.07−2.09/2.21 2.79−2.93/2.66−3.10/2.59−2.76 2.58/2.66/2.79 C2ν/C2ν/C2ν

6.35/7.65/7.06 −3.41/−3.54/−3.66 2.18−2.79/2.16−2.25/2.22−2.75 2.84−3.16/2.68−3.12/2.67−2.88 2.59/2.65/2.78 Cs/Cs/Cs

9.55/9.05/7.78 −0.84/−0.87/−1.32 2.00−2.18/1.91−1.94/2.01 2.75−2.91/2.57−2.92/2.31−2.67 2.60/2.66/2.79 C2ν/C2ν/C2ν

C


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Table 2. Adsorption Energy (E2ad) of O2, 2 × O, and CO, Bond Length of O2 (rOO) and CO (rCO) Molecules, Charge Transfer (Q) from the Adsorbent [Au7Cu23/MgO(100) or Au23Cu7/MgO(100)] to the Adsorbate (O2, 2 × O or CO), and Activation Energy Barrier (O2 → O + O) for the Lowest Energy Adsorption Systemsa E2ad(eV) O2

a

2×O

CO

defect-free F-center V-center

1.28 1.89 1.00

3.79 4.22 2.54

1.23 1.27 1.17

defect-free F-center

0.16 0.68

1.17 1.12

0.90 0.56

rOO (Å)

rCO (Å)

O2

CO

Au7Cu23/MgO(100) 1.46 1.19 1.51 1.19 1.44 1.19 Au23Cu7/MgO(100) 1.40 1.15 1.47 1.15

Q (e)

reaction (eV)

O2

2×O

CO

O2 → O + O

1.20 1.46 1.11

2.18 2.22 2.16

0.43 0.36 0.35

0.10, 0.43 0.13 0.32

0.89 1.18

1.84 1.89

0.08 0.08

0.69 0.62

O2 cannot adsorb on the Au23Cu7/MgO(100) system with V-center (missing).

Figure 2. Projected electronic density of states (PDOS) of the O2 adsorbed onto (a) Au7Cu23 and (b) Au23Cu7 clusters on the F-center MgO(100) support and zoom-ins near the Fermi energy for cluster atoms (insets). HOMO−1, HOMO, and LUMO levels of the gas phase triplet O2 molecule are included for reference in blue color. The PDOS are projected onto the O2 molecule and Au/Cu atoms of the Au7Cu23 and Au23Cu7 clusters. The Fermi energy is set at zero.

(missing row). The most stable adsorption configurations are given in Figure S1. The O2 molecules have similar adsorption configurations on Au7Cu23/MgO and Au23Cu7/MgO, where the molecule is rotated on the bridge site of a Cu−Cu and Au− Au bond, respectively, at the interface between the cluster and support. These differ considerably from the adsorption on Au15Cu15/MgO,27 where a Cu−Cu bond on the cluster facet is the preferable adsorption site (bridge site). The direct interaction with the substrate causes the charge transfer to O2 from Au7Cu23/MgO (1.11−1.46 e) and Au23Cu7/MgO (0.89− 1.18 e) to be more than that of Au15Cu15/MgO (0.68−0.84 e). For the CO molecule, the preferable binding sites involve Cu atoms on the cluster facet in each case (hollow, bridge, and top sites). The binding energy of CO is similar or stronger than that of O2 on the defect-free and V-center Au7Cu23/MgO(100) systems (Table 2). The defect-free Au23Cu7/MgO(100) system binds also CO more strongly than O2. This means that CO poisoning is a likely phenomenon for these catalysts. However, the clusters on the F-center prefer clearly to bind O2. Typically,

transfer relates to the electronic nature of defects, where the Fcenter stands out due to its two hosted electrons. In general, the larger electron negativity of Au (2.4 compared to 1.9 of Cu)52 yields that Au atoms are negatively charged, while Cu atoms are positively charged. 3.2. O2 and CO Adsorption Energies. Previously, it has been found for CO oxidation on free and supported Au clusters that the strong CO binding on Au hinders the adsorption of O2,53,54 leading to CO poisoning and a low reaction rate. In the case of the Au15Cu15/MgO model catalyst, we also confirmed that the cluster preferentially binds CO over O2.27 However, the Au7Cu3/CeO2 system has been reported to bind O2 more strongly than CO.55 Here, we examine all individual adsorption sites of Au7Cu23 and Au23Cu7 on MgO supports for O2 and CO adsorption. Table 2 shows the energies (E2ad) of O2 and CO binding on Au7Cu23 and Au23Cu7 with MgO supports. The adsorption energy of O2 is less than 0.01 eV for the Au23Cu7/MgO system with V-center, indicating no binding for the oxygen molecule D


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Figure 3. Side and top views of the charge density difference (CDD) of the adsorbed O2 molecule and HOMO/LUMO orbitals of the Au7Cu23 and Au23Cu7 clusters on MgO(100) with the F-center. The adsorbed O2 molecule is denoted in gray color. Blue and pink colors in CDD represent charge depletion and accumulation, respectively. The isosurface values are ±0.002 e/a03 for CDD and ±0.02 e/a03 for HOMO and LUMO.

PDOS, but the orbital is not completely localized. In addition, the d-band center (Cd) has been calculated to discern the difference in these two systems. The Cd values are −2.45 and −3.16 eV, respectively, for the O2 adsorbed Au7Cu23 and Au23Cu7 on the F-center (the corresponding value for Au15Cu15 is −2.89 eV, ref 27). 3.3. O2 Dissociation. As mentioned above, the adsorption and activation of O2 molecules are important steps in the CO oxidation reaction. It is known that O2 cannot dissociate on Au, since it exhibits large dissociation energy barriers.17,56,57 However, recent experimental and computational studies have shown that O2 can adsorb dissociatively on Cu clusters.51,58 Moreover, the O2 molecule can be effectively activated upon adsorption and dissociated to 2 × O atoms easily on Au15Cu15/ MgO(100).27 Thus, we investigated the dissociation of O2 on the most stable binding geometries of Au7Cu23/MgO(100) and Au23Cu7/MgO(100) with or without defects before examining the CO oxidation mechanisms. For the O2 dissociative adsorption, the total energy of the oxygen molecule (triplet state) was used as E(adsorbate) in eq 2 to take into account the correct spin state of the gas phase O2. The identified lowest-energy reaction paths for the O−O bond cleavage on Au7Cu23 and Au23Cu7 with the F-center supports are shown in Figure 4. For the defect-free and Vcenter supports, the corresponding reaction paths are given in Figure S4. The adsorption energy (E2ad) of the dissociated O2 (2 × O), bond length of O2 (rO−O), charge transfer (Q) to O2 and 2 × O, and activation energy barriers (O2 → O + O) for the most stable adsorption complex are listed in Table 2.

it is considered that the molecule with the larger adsorption energy is likely to preadsorb on the catalyst. Therefore, the Au7Cu23 and Au23Cu7 clusters on the F-center support appear to be promising catalysts for CO oxidation. To further understand the electronic structure upon O2 adsorption, Figure 2 gives the projected density of states (PDOS) of Au7Cu23 and Au23Cu7 on the F-center with an adsorbed O2 molecule. The HOMO and LUMO states of the gas phase triplet O2 molecule are also included for reference, and these are 2-fold degenerate, each. Upon adsorption of O2, an electron is transferred to the empty 2π* orbitals (LUMO) which is pulled down below the Fermi energy. This results in elongation of the O−O bond [1.51 and 1.47 Å (Table 2) versus 1.24 Å for the gas phase], and the molecule is activated to the superoxo O2− state. Interestingly, the electronic states involving oxygen are exactly at the valence band edge in Au23Cu7, while those for Au7Cu23 are shifted farther below the Fermi energy. There is no spin polarization for systems with O2 adsorption, which is different from our previous studies for the Cu20 cluster, where electron density is transferred from the Cu cluster to O2, causing local spin polarization.51 The visualizations of the charge density differences (CDD) and the HOMO and LUMO states for the O2 adsorption are displayed in Figure 3. Combined with the information in Figures 2 and 3, one can see the strong charge transfer for O2 and that the bonding at the cluster−support interface is due to the hybridization of the oxygen p states (from the molecule and MgO support) and d states of Au and Cu (see also Figures S2 and S3). The HOMO orbital of the Au23Cu7 system displays a significant contribution on O2, as suggested on the basis of E


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Figure 4. Structures of the initial state (IS), transition state (TS), and final state (FS) of the lowest identified pathways for O2 → O + O on Au7Cu23/MgO(100) and Au23Cu7/MgO(100) with the F-center and the energy changes with respect to the IS. The symbol “*” refers to the atom or molecule being adsorbed on the cluster.

Figure 5. Structures of the initial state (IS), transition state (TS), intermediate state (IM), and final state (FS) for the catalytic CO oxidation on Au7Cu23/MgO(100) with the F-center by the Langmuir− Hinshelwood (LH) mechanism and the energy changes with respect to the IS. The symbol “*” refers to the atom or molecule being adsorbed on the cluster.

The adsorption energies of O2 and 2 × O are higher on Au7Cu23/MgO(100) than those on Au23Cu7/MgO(100), which clearly correlates with the Cu content. The preferred adsorption patterns of 2 × O are hollow sites on Au7Cu23/ MgO(100) and Au23Cu7/MgO(100) with different supports (Figures 4 and S4). In each case, one oxygen atom binds between the cluster and the substrate interface, whereas there is variation with the location of the other one on the cluster facet. The dissociative adsorption is energetically preferred with more charge transfer (Table 2). Similar to the O2 case, the substrate affects the charge of the adsorbed oxygen atom at the interface. For Au7Cu23/MgO(100), the O2 and 2 × O adsorption energies are highest on the F-center and lowest on the V-center support. The calculated dissociative reaction barriers are very small on all supported clusters but in particular on the F-center (0.13 eV). Note that oxygen dissociation on the defect-free MgO support has two barriers, as shown in Figure S4. For Au23Cu7/MgO(100), the O2 adsorption energy is higher on the F-center, while the values are nearly the same for the 2 × O adsorption. The energy barrier is 0.62 eV for O2 dissociation on the F-center support. Although the barriers are higher than those on Au7Cu23/MgO and Au15Cu15/MgO (0.15 eV),27 they are still lower than the dissociation on Au catalysts (more than 1.0 eV).17 Obviously, alloying Au with Cu increases the binding of O2 and benefits the molecular dissociation. 3.4. Reaction Mechanisms for CO Oxidation. The clusters on the F-center are the only systems which clearly prefer to bind O2 more strongly than CO, and they also dissociate the O2 molecule readily. Therefore, these two systems are selected for a further study on CO oxidation. Both the Langmuir−Hinshelwood (LH) and Eley−Rideal (ER) mechanisms are considered,59 and the reaction paths with dissociated O atoms are also taken into account. The results of the reaction paths and energetics are displayed in Figures 5−7, S5, and S6. The LH reaction mechanism is initiated by the coadsorption of O2 and CO. The catalytic reaction pathways are shown in Figure 5 for the lowest energy coadsorption configurations on the Au7Cu23/MgO(100) system with an F-center. To compare the energies easily, the activation and reaction energies of different reaction pathways are summarized in Table 3. For O2* + CO*, the preferable coadsorption pattern involves the bottom CuCu site for O2 and the hollow (three Cu atoms) site for CO on Au7Cu23. The coadsorption energy is 3.09 eV (Table S1), which is comparable to the sum of single O2 and

Table 3. Calculated Activation Energy Barriers (Ef) and Reaction Energies (ΔH) for CO Oxidation on the F-Center Au7Cu23/MgO(100) and Au23Cu7/MgO(100)a Au7Cu23/MgO(100)

Au23Cu7/MgO(100)

reaction

Ef (eV)

ΔH (eV)

Ef (eV)

ΔH (eV)

CO* + O2* ↔ CO2 + O* CO* + O* ↔ CO2 CO* + O* + O* ↔ CO2 + O* CO + O2* ↔ CO2 + O* CO + O* ↔ CO2 CO + O* + O* ↔ CO2 + O*

0.21 0.52 0.35 0.14 0.29 0.31

−2.66 −0.11 −0.28 −3.89 −1.38 −1.49

0.27 0.77 0.53 0.30 0.42 0.29

−2.36 −2.03 −1.69 −3.39 −3.17 −2.76

The symbol “*” refers to the atom or molecule being adsorbed on the cluster. a

CO adsorption energies (3.16 eV) on the same system. The OO and CO bond lengths are not affected by the coadsorption (Table S1). After the initial adsorption, the LH reaction proceeds via a barrier (TS) of 0.21 eV to a metastable intermediate (IM) state. The OO and CO bonds are slightly elongated to 1.54 and 1.21 Å in the IM state. Subsequent to the IM complex, there is a barrierless release of the formed CO2 molecule. Co-adsorption of another CO at the closest bridge site with the remaining O atom (O* + CO*) leads to the formation of a second CO2 with a barrier (TS) of 0.52 eV (middle row). An IM state with weak bonding (0.08 eV) of CO2 is formed also in this reaction. The catalytic cycle is completed after this step. Alternatively, the first CO2 formation may involve a reaction with the predissociated O2. Upon the coadsorption of 2 × O* + CO* (bottom row), CO and the nearest O move closer to each other, followed by a crossing of the energy barrier (TS) to form the IM complex with an activation energy of 0.35 eV. After that, a CO2 molecule is released. The rest of the catalytic cycle repeats the step with a single oxygen, i.e., O* + CO* ↔ CO2. The ER mechanism involves an attack of a gaseous CO molecule on a preadsorbed O2 or 2 × O on Au7Cu23/ MgO(100) with an F-center. The role of the catalyst is determined mainly by its effect on O2. The reaction pathways and the calculated activation barriers are displayed in Figure S5 and Table 3. The abstraction of the first O atom from the O2 F


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The Journal of Physical Chemistry C molecule needs to overcome a very small energy barrier of 0.14 eV and the O−O bond is already broken in the TS, which stems from the high-degree activation of O2 upon adsorption on Au7Cu23. The activation energy barrier of TS increases to 0.29 eV for the abstraction of the second O atom. For the 2 × O* + CO reaction, the TS barrier is 0.31 eV for the first CO2 molecule release. For the Au23Cu7/MgO(100) system with an F-center, similar reaction steps are considered. Figure 6 displays the LH reaction

Figure 6. Structures of the initial state (IS), transition state (TS), and final state (FS) for the catalytic CO oxidation on Au23Cu7/MgO(100) with the F-center by the Langmuir−Hinshelwood (LH) mechanism and the energy changes with respect to the IS. The symbol “*” refers to the atom or molecule being adsorbed on the cluster.

pathways. The values of the activation barriers are also included in Table 3. In this case, CO adsorbs on the top Cu site and O2 binds to the bottom Au−Au site. The coadsorption energy of O2* + CO* is higher than the sum of the single O2 and CO adsorption energies by 0.40 eV (Table S1), which means that the coadsorption system is energetically lower than those of the individual adsorbates. Upon the coadsorption of CO and O2, the molecules move closer to each other, followed by the breaking of the O−O bond with the activation energy barrier (TS) of 0.27 eV to form the first CO2 molecule. After the first CO2 molecule release, the coadsorption of a new CO molecule leads to formation of another CO2 with a barrier of 0.77 eV (middle row). The resulting CO2 gets effectively ejected out from the cluster. After this step, the catalytic cycle for CO* + O2* is completed. For the dissociated O2 (bottom row), CO adsorbs on the top Au site and the corresponding TS has an activation energy of 0.53 eV. The process continues as described for a single oxygen atom (middle row). Figure S6 displays the ER reaction pathways, and the corresponding energy barriers are also listed in Table 3. The abstraction of the first oxygen atom in the reaction O2* + CO needs to overcome an energy barrier of 0.30 eV. The O2 bond length is elongated to 1.67 Å in TS, while the CO bond is hardly influenced. The subsequent step is CO oxidation with the remaining O atom. The corresponding barrier is 0.42 eV. Furthermore, the barrier for the reaction with the dissociated O2 (2 × O* + CO) is 0.29 eV. The potential energy diagrams of CO oxidation with all the reaction pathways analyzed above are plotted in Figure 7. The corresponding reaction pathways for the Au15Cu15/MgO(100) system with an F-center are also included for comparison. The

Figure 7. Potential energy diagrams of CO oxidation for the (a) Au7Cu23/MgO(100), (b) Au15Cu15/MgO(100), and (c) Au23Cu7/ MgO(100) systems (on F-centers) by the LH and ER mechanisms. The corresponding reaction pathways for O2 (pre-) dissociation are inserted in each panel.

exothermic nature of the CO oxidation process is clearly demonstrated with the formation of two CO2 molecules, and the interesting aspects involve the evolution of reactions in each case. The results show a strong adsorption for the Cu-rich cluster, and the energy deviation among different reactants decreases with increasing Au:Cu ratio. For Au7Cu23 and G


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F-center prefer to bind O2 more strongly than CO. We use the condition P(CO) = 0.01 bar with different O2 partial pressures combined with T = 150 and 300 K in the microkinetic model to evaluate catalyst coverages and the rate of CO2 formation at longer time scales. The results are collected in Table 4.

Au15Cu15, the adsorption energy of 2O* + CO (ER channel) is lower than that of O2* + CO*, while it is the reverse for Au23Cu7. Correspondingly, the dissociation barriers of the O2 molecule (figure insets) increase as the Au content increases. These results indicate that Cu-rich alloys may exhibit overbinding of reactants (Table S1), and this can block CO oxidation. In particular, Cu is prone to O atoms which is related to its notorious oxidation properties. Generally, the reaction barriers for CO oxidation are small on the AuCu/MgO systems with the F-center defect. The LH mechanism is lower in energy overall due to the adsorption energies of both CO and O2 (or 2 × O), while the ER mechanism is missing the CO adsorption component. The strong binding of oxygen on Au7Cu23 results in the energy being already rather close to the final level after the first CO2 formation, whereas Au23Cu7 is only halfway through. The CO oxidation barriers on the Au15Cu15 cluster are mostly lower than those on the other two systems, especially for the ER reaction pathways. This can be understood further by inspecting the PDOS upon O2 adsorption (Figure S7) which shows strong weight on oxygen at the Fermi energy and its contribution on both sides of the narrow band gap. This indicates increased reactivity for adsorbed O2 and explains the low barrier for approaching CO. The above results show that the AuCu alloys are good catalysts for CO oxidation. However, the choice of the Au:Cu ratio has important consequences for the catalytic activity, which will be shown more clearly in the microkinetic modeling below. We remark that we have focused here on low O2 and CO concentrations and we have not studied the effect of several oxygen molecules or oxidation. Higher reactant coverages would require an enormous number of configurations, and such computations are out of the content of this study. 3.5. Microkinetic Model. On the basis of the DFT calculations, a seven-step microkinetic model27,60 was developed to further investigate the activity of the Au7Cu23/ MgO(100) and Au23Cu7/MgO(100) catalysts on F-centers. In comparison to the molecular reaction studied above, the microkinetic model is a simplification, which ignores the two predissociated O* containing reactions and atomistic details of the reactions. However, this model enables us to incorporate real experimental variables, such as partial pressures and temperatures. Moreover, the model complements the DFT calculations by including average surface coverage effects. The elementary steps and full details of the model have been described already in ref 27. Although there is no direct experimental data for CO oxidation on MgO-supported AuCu clusters, CO oxidation on MgO-supported Au clusters has been studied extensively.13,14 Especially, Yoon13 et al. found that CO2 was produced at 140 and 280 K on F-center-rich Au8/MgO(100) thin films. Moreover, Henkelman et al.55 studied several Au-based bimetallic nanoclusters and found that the CeO2(111)supported Au7Cu3 cluster is optimal for catalyzing CO oxidation, and the microkinetic model clearly indicates a higher activity for the AuCu catalyst under the condition of T = 298 K, P(CO) = 0.01 bar, and P(O2) = 0.21 bar. Our previous study also shows that P(CO) = 0.01 bar is the most beneficial choice for CO2 production on the Au15Cu15/MgO(100) system with an F-center.27 However, the stronger CO binding on Au15Cu15 leads to CO poisoning of the cluster surface for similar partial pressures of CO and O2. Here, the situation is different, as the Au7Cu23/MgO(100) and Au23Cu7/MgO(100) systems with an

Table 4. Calculated Coverage of Species (θCO, θO2, θO) and Rate (s−1) of CO2 Formation (rCO2) at Long Time Scales with Different Temperatures (150 and 300 K) and O2 Partial Pressures under P(CO) = 0.01 bar Au7Cu23/MgO(100) 150 K

300 K

Au23Cu7/MgO(100) 150 K

300 K

θCO θO2

1.0 5.71 × 10−22

P(O2) = 0.01 bar 3.67 × 10−1 1.26 × 10−1 −4 5.54 × 10 5.56 × 10−7

θO rCO2

1.15 × 10−16 1.14 × 10−15

6.32 × 10−1 1.05 × 106

8.73 × 10−1 3.90 × 10−4

7.79 × 10−1 1.00 × 104

θCO θO2

5.64 × 10−1 3.15 × 10−6

P(O2) = 0.05 bar 3.74 × 10−2 2.45 × 10−4 −3 2.30 × 10 7.38 × 10−5

7.81 × 10−4 7.56 × 10−3

θO rCO2

4.35 × 10−1 4.83

9.58 × 10−1 1.59 × 106

9.99 × 10−1 4.72 × 10−4

9.84 × 10−1 1.06 × 104

θCO θO2

2.50 × 10−1 6.10 × 10−6

P(O2) = 0.1 bar 1.66 × 10−2 1.08 × 10−4 2.64 × 10−3 8.30 × 10−5

3.47 × 10−4 8.49 × 10−3

θO rCO2

7.49 × 10−1 8.31

9.78 × 10−1 1.62 × 106

9.99 × 10−1 4.72 × 10−4

9.82 × 10−1 1.06 × 104

θCO θO2

4.46 × 10−2 8.45 × 10−6

P(O2) = 0.5 bar 3.05 × 10−3 2.00 × 10−5 2.92 × 10−3 9.04 × 10−5

6.38 × 10−5 9.24 × 10−3

θO rCO2

9.53 × 10−1 1.05 × 101

9.91 × 10−1 1.65 × 106

9.81 × 10−1 1.06 × 104

9.99 × 10−1 4.72 × 10−4

2.21 × 10−1 1.04 × 10−4

Table 4 shows that the rate of CO2 formation increases significantly with temperature increase from 150 to 300 K for both systems. Interestingly, at higher O2 partial pressures, the coverage of O is high, while that of O2 and CO remains negligible. This can be understood in terms of the DFT calculations where O2 binding is stronger than that of CO and O2 dissociates rather readily to O atoms on these two systems. Moreover, the CO2 formation is saturated when the O2 partial pressures are increased. On the basis of these observations, we chose CO and O2 with the same partial pressure of 0.01 bar and T = 300 K to investigate further the CO2 formation on these two systems. Figure 8 shows the coverages of reactant species (O2, CO, O) and the turnover frequency (TOF) of CO 2 from microkinetic model simulations as a function of time for Au7Cu23/MgO(100) and Au23Cu7/MgO(100) at P(CO) = 0.01 bar, P(O2) = 0.01 bar, and T = 300 K. Throughout the process, the coverage of O remains at a relatively high level, while the coverage of O2 is negligible for both systems. The O2 molecules dissociate immediately after adsorption, or they are rapidly consumed in the CO oxidation processes. The CO overage is saturated at a moderate level, and the steady state is reached with CO2 production. While the trends for CO2 production are different for the two cases, the TOF of the CO2 production is still pronounced for Au23Cu7/MgO(100). On the other hand, high oxygen coverages may cause oxidation H


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(Mg-vacancy) MgO(100) supports. The support induces negative charge transfer to the Au7Cu23 and Au23Cu7 clusters in all cases, and the effect is pronounced for the F-center. The alloy composition turns out crucial in terms of the reactant adsorption energies and sites, selectivity (possible poisoning), and reaction barriers. These effects are amplified in the reaction kinetics and sensitivity to external parameters (microkinetic modeling) highlighting the possibility for catalyst design in terms of bimetallic alloy composition. The adsorption of O2 and CO has been calculated by tuning the location of vacancies in MgO(100). Here, the only systems binding O2 more strongly than CO are Au7Cu23/MgO(100) and Au23Cu7/MgO(100) with the F-center. The interfacial binding of O2 in the AuCu/MgO perimeter strengthens the substrate effect by inducing more charge transfer to O2. Moreover, O2 can be effectively activated upon adsorption and dissociated to 2 × O atoms by crossing a low energy barrier, especially on the F-center support. The O2 dissociation barrier decreases for Cu-rich alloys. CO oxidation reaction paths have been explored on the basis of the LH and ER mechanisms, and the dissociated O atoms are also taken into account for the reaction paths. In general, the reaction barriers for CO oxidation are small for the clusters on F-centers, and the LH mechanism is lower in energy overall than ER due to the coadsorption of CO and O2 (or 2 × O). The increased Cu content causes overbinding of reactants which may turn out harmful for CO oxidation in more realistic conditions (e.g., oxidation). The microkinetic modeling built on the collected DFT results confirms that the CO2 production rate is significant for the F-center Au7Cu23/MgO(100) and Au23Cu7/MgO(100) systems at low temperature (300 K). In comparison with the Au15Cu15/MgO(100) system,27 the sequence of the CO2 production rate is r(Au15Cu15) > r(Au7Cu23) > r(Au23Cu7). While the CO2 production is the highest for Au15Cu15, it is also very sensitive to CO poisoning (strong CO binding). For Au7Cu23 and Au23Cu7, the stronger binding of O2 than that of CO modifies the catalyst sensitivity toward CO and O2 partial pressures. We note that our model does not take into account possible reoxidation of F-centers which may become relevant at high temperatures as the cluster mobility increases. However, this is not an issue at low T, as shown by the experiments for Au8 clusters.13 Altogether, we find that the catalyst composition (Au:Cu ratio), the catalyst structure (location of Au and Cu), the support and its structure (defects), and the interfacial effects on adsorption have deep influences on the catalytic performance of supported bimetallic AuCu nanoparticles. The catalytic process is a complex problem, which needs to be studied case by case by taking into account these factors.

Figure 8. Coverages of the reactant species (O2, CO, O) and TOF of CO2 from microkinetic model simulations on (a) Au7Cu23/MgO(100) and (b) Au23Cu7/MgO(100) with the F-center as a function of time [P(CO) = 0.01 bar, P(O2) = 0.01 bar, T = 300 K].

of Cu sites in Cu-rich clusters, and redox reactions may also occur during the CO oxidation process. Finally, we note that the MgO support with the F-center defect is crucial for catalytic activity. As shown in detail for the Au15Cu15/MgO system,27 the rate of CO2 production is very low on the defect-free or V-center MgO supports. In addition, the Au:Cu ratio influences the reaction conditions and the CO2 production. For Au15Cu15, we observe CO oxidation activity already at 150 K,27 while there is almost no CO2 production for Au7Cu23 and Au23Cu7. As the temperature is increased to 300 K, the production of CO2 increases markedly for all three compositions. Remarkably, the CO2 production rate of the Au15Cu15 catalyst (∼107 s−1) is 10 times faster than that of Au7Cu23 (∼106 s−1), while the latter is 2 orders of magnitude faster than the Au23Cu7 (∼104 s−1) catalyst. However, the CO2 production of Au15Cu15 is very sensitive to the CO partial pressure, as the CO binding energy is higher than that of O2. For Au7Cu23 and Au23Cu7, the interface adsorption effect leads to the stronger binding of O2, which modifies the sensitivity of the catalyst to CO and O2 partial pressures.

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ASSOCIATED CONTENT

S Supporting Information *

The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acs.jpcc.6b12054. Properties of the most stable coadsorption configurations (Table S1); most stable O2 and CO adsorption configurations (Figure S1); PDOS of the Au7Cu23 and Au23Cu7 clusters on the F-center MgO(100) supports (Figure S2); CDD of the Au7Cu23 and Au23Cu7 clusters adsorbed on F-center MgO(100) supports (Figure S3); pathways of O2 dissociation on Au7Cu23/MgO(100) with the defect-free and V-center surfaces and Au23Cu7/

4. CONCLUSION We have reported findings for the CO oxidation mechanisms on the MgO-supported AuCu clusters based on DFT simulations and microkinetic modeling. We place particular focus on the effect of the Au:Cu ratio which we have now mapped for three compositions (1:3, 1:1, 3:1) for the particular cluster size of N = 30. We have systematically considered the clusters on the defect-free, F-center (O-vacancy), and V-center I


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MgO(100) with the defect-free surface (Figure S4); CO oxidation on Au7Cu23/MgO(100) and Au23Cu7/MgO(100) with the F-center surfaces by the ER mechanism (Figures S5 and S6); and PDOS of the O2 adsorbed Au15Cu15 cluster on the F-center MgO(100) support (Figure S7) (PDF)

AUTHOR INFORMATION

Corresponding Author

*E-mail: jaakko.akola@tut.fi. Phone: +358 40 198 1179. ORCID

Kari Laasonen: 0000-0002-4419-7824 Jaakko Akola: 0000-0001-9037-7095 Notes

The authors declare no competing financial interest.

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ACKNOWLEDGMENTS The DFT calculations were carried out in CSC - the IT Center for Science Ltd., Espoo, Finland. Financial support has been provided by the Academy of Finland through its Centre of Excellence Program (Project 284621) and the European Union Horizon 2020 NMP programme through the CritCat Project under Grant Agreement No. 686053.

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Catalytic Activity of AuCu Clusters on MgO(100) - ACS Publications

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